The magnetic field at the centre of a wire loop formed by two semicircular wires of radii $r_1=3.14 \mathrm{~m}$ and $r_2=6.28 \mathrm{~m}$ and carrying a current of $\mathrm{I}=2 \mathrm{~A}$ is:
$6 \times 10^{-7} T$
$2 \times 10^{-7} T$
$3 \times 10^{-7} T$
$4 \times 10^{-7} T$
Two vessels A and B contain same mass of Oxygen and Hydrogen respectively at the same temperature. The volume of $B$ is twice that of $A$. The ratio of gas pressure in $A$ to that in $B$ is
1: 8
1:64
1:256
1:32
Two conducting spherical shells $A$ and $B$ of radii 4 cm and 6 cm respectively are placed with their centres 17 cm apart in air. Initially, sphere A was given a -20 nC charge while sphere B was uncharged. The spheres are then connected by a long thin conducting wire and allowed to reach electrostatic equilibrium. Assuming no charge is lost to the surroundings, the final charge on sphere A and the ratio of magnitude of electric field intensity at the surface of sphere $B$ to that of sphere $A$ is given by;
$-12 \mathrm{nC} ; \frac{2}{3}$
$-8 \mathrm{nC} ; \frac{3}{2}$
$-12 \mathrm{nC} ; \frac{3}{2}$
$-8 \mathrm{nC} ; \frac{2}{3}$
A uniform electric field $E=3 \hat{i}+6 \hat{j}+\hat{k}$ passes through a closed cuboidal surface. One face of the cuboid has an area $4 m^2$ and an outward unit normal given by $\frac{2 \hat{i}+2 \hat{j}+3 \hat{k}}{\sqrt{17}}$. If the electric flux through the remaining 5 faces is zero, the charge enclosed by the cuboid is:
Cannot be determined
$\frac{84 \epsilon_0}{\sqrt{17}}$
zero
$\frac{\sqrt{17}}{84 \epsilon_0}$
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